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Gamma Ray Bursts from Binary Black Holes

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Gamma Ray Bursts from Binary Black Holes Gamma ray bursts from binary black holes Agnieszka Janiuk Center for Theoretical Physics, Polish Academy of Sciences, Warsaw Collaboration: Szymon Charzyński (Warsaw University) Michał Bejger (Copernicus Astronomical Center, Warsaw) www.cft.edu.pl A&A, 2013, 560, 25 Gamma Ray Bursts Prompt emission in Gamma, late-time emission with X-rays Energetic explosions connected with collapse of massive stars or compact object mergers Especially interesting is scenario when two compact objects merge within a collapsar Electromagnetic signal accompanied by gravitational waves We unify the two “standard” models Massive star explosion and mass fallback from the envelope Paczyński (1998); McFadyen & Compact binary merger: neutron Woosley (1999) star disruption Eichler et al. (1989); Ruffert & Janka (1999) Compact companion enters the massive star's envelope Common envelope phase, transient phase (analog of a Thorne-Żytkov object) Trigger of the core collapse, SN (Hypernova) explosion -> GRB Ultimate fate of HMXBs: Binary pulsar NS-BH BH-BH Possible progenitors: known high mass X-ray binaries Close binary: massive OB star plus compact remnant Examples: Cyg X-3, IC 10 X-1, NGC 300 X-1, M33 X-7 Statistics: the advanced LIGO/VIRGO detection rate of BH-BH mergers from Cyg X-3 formation channel is estimated at 10 yr-1 BH HMXBs formed at z>6 might have impact on cosmic reionisation. Their Zhang & Fryer (2001); Barkov & fraction should increase with redshift Komissarov (2010); Church et al. (2012); Belczyński et al. (2013); Mirabel et al (2011) Our scenario Close binary: massive OB star plus compact remnant (BH) We consider four phases: (1) Massive star is spun up by the interaction in binary system and then by the orbiting BH inside the envelope (2) Core collapse and accretion of inner envelope, evolution of primary BH mass and spin (3) Binary black hole merger (4) Final accretion of the envelope onto the merger product Model of pre-supernova star Pre-supernova star (Woosley & Weaver 1995) Enclosed mass of 25 MSun Density distribution: chemical composition of an evolved star (Fe, Si, C, O, He, H) Iron core of mass 1.4 MSun Spinning up the envelope and core black hole We adopt specific angular momentum distribution in the star (differential rotation) l spec r ,=l0 1−∣cos∣ The infalling envelope matter adds mass and spins the black hole. The rotationally supported torus must obey (Bardeen et al. 1972): 2G M BH l specl crit= 2−a21−a c This condition depends on time; AJ & Proga (2008); AJ, Moderski & Proga (2008) Mass of the envelope shell during the collapse (green:total; red: contained in the rotating torus). The three lines show the models with various normalisation of the specific angular momentum in the envelope: x=1.5 (solid), x=3.0 (dashed) and x=7.0 (dotted). Mass loss through the wind Wolf-Rayet stars: mass loss of 10-5 M /yr (e.g., Dwarkadas 2013) sun Mass loss in MHD simulations: McKinney et al. (2006); Kumar et al. (2008); AJ, Mioduszewski & Mościbrodzka (2013); AJ & Kamiński (2014); See also: Proga (2004; 2007); Miller et al. (2006); AJ, Grzędzielski & Capitanio (2014, in prep.) → AGN/X- ray binaries winds from accreting BHs Spinning up the envelope and core black hole The companion BH transfers the specific angular momentum dJ M G r r l= 2 = 2 1ln 2 dM 2 M r r Torus accretion: BH spins up to maximum rate. Some (most ?) of its mass will be lost in wind. Evolution scenarios We proposed two representative scenarios for the pre-merger configuration Homologous accretion of the total envelope, when both the rotating torus and material from the poles contribute to the growth of the primary black hole Only torus accretion, while the material from the poles is expelled. Some torus mass might further be expelled through winds The primary BH grows in mass to about ~3 – 9 M . Sun This phase may last up to ~500 s (first jet emission). Then the secondary BH sinks to merge with it. The spin of the primary at merger time is above ~0.7. www.einsteintoolkit.org Merging two black holes Numerics done with Cactus Computational Toolkit (Goodale et al. 2003; Loeffler et al. 2012) 3+1 split of Einstein equations; Cauchy initial value problem solved with BSSN method (Shibata & Nakamura 1995; Baumgarte & Shapiro 1999) 3D Cartesian grid; adaptive mesh, reflection symmetry Interdisciplinary Center for assumed to reduce number of Mathematical and Computational Modeling, grid points and computer Warsaw University requirements We track numerically the very last stage of BBH merger: initial separation of 6M; inspiral, merger and ringdown Quasicircular orbits, mass ratio q=1-3 Primary spin a=0-0.9, directed perpendicularly to orbital plane Secondary is spinless Apparent horizons of the binary BH components during merger Parameters: m = 0.632, m = 0.316, s =0.9 1 2 1 ADM mass ratio M /M = 3.0 1 2 Resulting final ADM mass and dimensionless spin M = 1.34, a = 0.76 3 3 Gravitational recoil Total linear momentum radiated from the system through gravitational waves is computed through the coefficients Alm of multipole expansion of the Weyl scalar (Alcubierre 2008). Recoil vector remains in the orbital plane, because we assumed reflection symmetry; in general, it does not have to be the case We obtained velocity of the product, depending on spins and mass ratio of components, 200-300 km/s Accretion of the remaining matter onto merged hole Magnetic fields transfer the rotational energy of the black hole to the polar jets Observational perspectives Large recoil speed for q~1 (for primary BH mass small due to wind taking most of envelope's), the offset of GRB afterglow is possible The merger product would leave the GRB host galaxy if v~2000 km/s. Possible if both BHs have extremely large spins (Tichy & Maronetti 2007). Theoretical perspectives Recoil kick directed into circumbinary disk plane can alter the distribution of specific angular momentum (Rossi et al. 2010). If magnetic fields are involved, expansion of dual jets driven by generalized Blandford-Znajek mechanism (Palenzuela et al. 2010) Summary ➢ The long duration GRB may originate from a merger of a close compact binary system, containing a high mass evolved star and a black hole. ➢ The event can be divided into stages: Onset of the core collapse in the primary star, connected with the tidal interaction with secondary black hole. The inner shells of the envelope are spun up by the companion, and accrete onto the primary BH, increasing its mass and rotation spin The merger of two black holes, surrounded by a circumbinary torus; gravitational waves; kick Accretion of a remnant mass onto the BH merger product ➢ Possible observational consequences Electromagnetic signal from the jets, POSSIBLY DOUBLE Gravitational wave signal in between the jets Possible delay and offset of the second GRB signal (or its afterglow emission), due to recoil Possible precession/interaction between two jets flows if redirected Now you are welcome to the jungle of black hole binaries that tend to have a huge appetite for destruction... So let us jump to the paradise city of numerical simulations where it's so easy to say that 'anything goes'.
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